Titlebook: Optical Bistability 2; Charles M. Bowden,Hyatt M. Gibbs,Samuel L. McCall Book 1984 Springer Science+Business Media New York 1984 atoms.bif

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Zeeman Coherence Effects in Absorptive Polarization Bistabilityntly, attention has been paid to OB in three-level systems.. Here, the physical process of transverse optical pumping,. related to coherent population trapping, plays an important role. Of particular interest is the case of J = 1 → J = 0 transition of an atomic system wherein orthogonally circular-p

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Polarization Switching with Sodium Vapor in a Fabry Perotitching and hysteresis in the polarization state of the output as one varied the input power. Their model was subsequently generalized to include saturation effects [2] and a model was developed using a more realistic atomic model, the J = 1/2 to J = 1/2 transition [3]. Furthermore, it has been pred

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Optical Bistability, Chaos in the Coherent Two Photon Processes a two photon transition.. Maxwell-Bloch equations are used to obtain the input vs. output relation by adiabatically eliminating all the atomic variables. The fundamental equation that results is a complex two dimensional map--which in the mean field limit reduces to the standard bistability equatio

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Self-Pulsing, Breathing and Chaos in Optical Bistability and the Laser with Injected Signaln the framework of the plane-wave, ring cavity model and the realization by McCall. of an electro-optical converter of cw coherent light into pulsed radiation. In a subsequent important development, Ikeda. showed that, in the dispersive case, the Bonifacio-Lugiato instability leads to chaotic behavi

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